steff (with upgrade for ear2)
DESCRIPTION
STEFF (with upgrade for EAR2). 3m. Fragment mass measurement. Time-of-flight -> velocity Bragg Ionisation chamber->energy Mass resolution 4 amu. Digital Bragg Pulse Processing. Digital Pulse Processing: High -pass filter Ballistic Def. Correction. Integration - PowerPoint PPT PresentationTRANSCRIPT
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STEFF (with upgrade for EAR2)
3m
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Fragment mass measurement
• Time-of-flight -> velocity • Bragg Ionisation chamber->energy• Mass resolution 4 amu
2
2EA
v
1 2
2 1
A v
A v
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Digital Bragg Pulse Processing
• Integration• Low-pass filter: noise reduction• Currently Noise ~0.2 percent
• Digital Pulse Processing:• High-pass filter• Ballistic Def. Correction
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Nuclear charge distribution for light mass groupIC measurements, when velocity if fixed:
Where
before any corrections:Sensitivity to Z (FWHM) of about 2 units.
b = 2/3
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Gamma-ray Energy and Multiplicity
• Response to NEA High Priority Request of more accurate knowledge of heating caused by gamma emission in the next generation of nuclear reactors
• Coincidence with emission of prompt gamma rays as a function of the fragment mass and energy
• 12 NaI detectors around the uranium target provide a 6.8% photo peak detection efficiency
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Gamma decay of fission fragment
Spin linked to g multiplicity and feeding by statistical models.Spin alignment to g-ray angular correlations
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235U Single g Energy distribution (ILL)
•Time random coincidences removed•Multiple-hit effects removed (GEANT4)
• Deconvolution (Compton/Backscatter, etc. removal) using GEANT4 response functions.
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Using GEANT4 simulations of response functions of NaI detectors
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Fragment Angular Distributions
Constrains calculations of fission barrier. STEFF: Anisotropy with A,Z,E* ?
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Rate Calculation for STEFF@EAR2
• Target 25cm2 235U at• Beam flux • Neutron energy range 1eV - 10 MeV• protons (~30 days running time)• Intrinsic Fragment detection efficiency 0.5*• Fragment-gamma events with A,Z,E• 5.6 fissions per pulse in 3ms†; Δtγ~15ns
-2cm100 g-1-26 s4.0cmn1054.7
*For both fragments. Limited by efficiency of STOP : to be improved. S.Warren PhD project.† charge collection in anodes in ~3us.
183 10
55 10
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STEFF Proposal Objectives
• To move STEFF to a EAR2 to study neutron-induced fission.• Measurement of E,A,Z and directions of fragments.• Use gamma multiplicities and angular distributions to look at
spin effects.• Meet NEA high-priority request for gamma-ray data.• Study fragment angular distributions vs. A,Z and E (Ex).
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Monte Carlo simulation (decay)
• Number of yrast gamma rays linked to mean spin ~ B.
• Geometric distributions give statistical gamma rays for each fragment.
• Interaction with array: ,e scattering
Probability of spin state is generated based statistical model:
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Characteristics of bragg pulse
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STEFF @ ILL
• Installed in pf1b Institut Laue-Langevin, Grenoble for 2x 25 days• 235U target 100µgcm-2 on a Nickel backing• Thermal neutron flux 1.8x1010 neutrons cm-2s-1
• Measured mass resolution 4 amu
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Design
2-Energy, 2-velocity Spectrometer.
Solid angle 60 mstr